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\@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{2}{section.1}}
\newlabel{sec:introduction}{{1}{2}{Introduction}{section.1}{}}
\@writefile{toc}{\contentsline {section}{\numberline {2}Samples}{3}{section.2}}
\newlabel{sec:samples}{{2}{3}{Samples}{section.2}{}}
\@writefile{toc}{\contentsline {section}{\numberline {3}Flow}{4}{section.3}}
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\newlabel{fig:v2_vs_n_all}{{3}{5}{Flow}{section.3}{}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces This figure reveals the relationship between v2 and number of collisions. The red the v2 of partons in their mediem state. The x-axis for the red line is the number of intermediate stage of collisions. That means a paron maybe recorded several times. For example, if a parton has 2 collisions before formations. The v2 of this parton will be recorded at $N_{Coll}^{*}=0,1,2$. This number will be defined as $N_{coll}^{*}$ to differ with $N_{coll}$, which is the x-axis of the black line. It means the total number of collisions of a certain parton. The dashed line is more complex, it means the partons in intermediate statge but not the final stage.}}{5}{figure.1}}
\newlabel{fig:v2_n_noptcut}{{1}{5}{This figure reveals the relationship between v2 and number of collisions. The red the v2 of partons in their mediem state. The x-axis for the red line is the number of intermediate stage of collisions. That means a paron maybe recorded several times. For example, if a parton has 2 collisions before formations. The v2 of this parton will be recorded at $N_{Coll}^{*}=0,1,2$. This number will be defined as $N_{coll}^{*}$ to differ with $N_{coll}$, which is the x-axis of the black line. It means the total number of collisions of a certain parton. The dashed line is more complex, it means the partons in intermediate statge but not the final stage}{figure.1}{}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces The differencial distribution of number of collision in different $P_{T}$ region. The distributions including different initial (drawn in dashed lines) or final (drawn in solid lines) $P_{T}$ shreshold. The black lines mean low $P_{T}$ region, where $P_{T}<0.5GeV$ and red lines mean high $P_{T}$ region, where $P_{T}>3GeV$, for both initial and final $P_{T}$ cuts.}}{6}{figure.2}}
\newlabel{fig:ncoll}{{2}{6}{The differencial distribution of number of collision in different $P_{T}$ region. The distributions including different initial (drawn in dashed lines) or final (drawn in solid lines) $P_{T}$ shreshold. The black lines mean low $P_{T}$ region, where $P_{T}<0.5GeV$ and red lines mean high $P_{T}$ region, where $P_{T}>3GeV$, for both initial and final $P_{T}$ cuts}{figure.2}{}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces v2 of partons in their final states as a function of total number of collision in different final $P_{T}$ region. The black line is v2 distribution of all the partons. And red, green and blue lines show partons with low, medium and higt final state energy respectively.}}{7}{figure.3}}
\newlabel{fig:v2_vs_N}{{3}{7}{v2 of partons in their final states as a function of total number of collision in different final $P_{T}$ region. The black line is v2 distribution of all the partons. And red, green and blue lines show partons with low, medium and higt final state energy respectively}{figure.3}{}}
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces These figure shows relationship of v2 and parton final $P_{T}$, The black line is the v2 distribution of all partons. In order to bettter analysis it, we split the sample based on the number of collisions. v2 vesus $P_{T}$ of different number of collisions are drawn with different color lines.}}{7}{figure.4}}
\newlabel{fig:v2_vs_pt}{{4}{7}{These figure shows relationship of v2 and parton final $P_{T}$, The black line is the v2 distribution of all partons. In order to bettter analysis it, we split the sample based on the number of collisions. v2 vesus $P_{T}$ of different number of collisions are drawn with different color lines}{figure.4}{}}
